1980
DOI: 10.1016/0029-554x(80)90116-0
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A thick-target radiation transport computer code for low-mass heavy ion beams

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Cited by 22 publications
(3 citation statements)
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“…2. The projectile ion energy loss by atomic ionization and excitation is determined by scaling the stopping values for protons, as described in Ref.…”
Section: Uwmentioning
confidence: 99%
“…2. The projectile ion energy loss by atomic ionization and excitation is determined by scaling the stopping values for protons, as described in Ref.…”
Section: Uwmentioning
confidence: 99%
“…These upper limits amount to roughly 1 GeV/nucleon, and even the adequacy of this number has uncertainty to it (Ref. 24, p. 162) since enough experiments have not been done to substantiate the theory; hence, we give only one upper limit, rather than both an "adequate" and a " best" upper limit.…”
Section: Fe(r) =El/(27r)!2](e) E-[t-r(e ]/A(e)mentioning
confidence: 99%
“…2. The major codes are the SAIC version [5] of HETC [6] for nucleon-meson transport, EGS [7] for simulating electromagnetic cascades, MORSE [8] for low-energy ( < 20 MeV) neutron transport, and the GAMA code [9] for de-excitation y-ray spectra from spallation collisions. The simulations follow the transport history of photons in the energy range from -100 GeV down to -0.1 keV due to gamma-ray sources from neutral pion decay, high-energy (spallation) collisions, and low-energy neutron inelastic scattering and capture reactions.…”
Section: Monte Carlo Simulation Methodsmentioning
confidence: 99%